DESIGN STUDY OF MEDICAL CYCLOTRON SCENT 300 Mario

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DESIGN STUDY OF MEDICAL CYCLOTRON SCENT 300 Mario Maggiore on behalf of R&D Accelerator

DESIGN STUDY OF MEDICAL CYCLOTRON SCENT 300 Mario Maggiore on behalf of R&D Accelerator team Laboratori Nazionali del Sud Catania, Italy HIAT 2009, 9 th June , Venice 1

CYCLOTRONS PROVIDING LIGHT IONS SYNCHROTRONS are today used everywhere (japan, GSI, CNAO) for carbon

CYCLOTRONS PROVIDING LIGHT IONS SYNCHROTRONS are today used everywhere (japan, GSI, CNAO) for carbon beam therapy IBA C 235 RESISTIVE COILS CYCLOTRONS SC CYCLOTRON PROTONS ACCELVARIAN K 250 SC IBA C 400 PROTONS INFN SCENT 300 CARBON IONS ü compactness and simplicity ü lower size and cost superconducting tech. ü high beam modulation control fixed energy (ESS needed) HIAT 2009, 9 th June , Venice 2

HIAT 2009, 9 th June , Venice 3

HIAT 2009, 9 th June , Venice 3

MAIN PARAMETERS HIAT 2009, 9 th June , Venice 4

MAIN PARAMETERS HIAT 2009, 9 th June , Venice 4

INJECTION LAYOUT Einj=25 AKe. V Vinflect= 14 KV gapinflect= 6 mm Einflect= 23 KV/cm

INJECTION LAYOUT Einj=25 AKe. V Vinflect= 14 KV gapinflect= 6 mm Einflect= 23 KV/cm Vdee inj=70 k. V Bo=3, 15 tesla ECR sources HIAT 2009, 9 th June , Venice 5

CENTRAL REGION DESIGN Beam centering YC XC Energy gain Vertical focusing during first turns

CENTRAL REGION DESIGN Beam centering YC XC Energy gain Vertical focusing during first turns 250 AKe. V/turn HIAT 2009, 9 th June , Venice 6

MAGNETIC FIELD PROPERTIES HIAT 2009, 9 th June , Venice 7

MAGNETIC FIELD PROPERTIES HIAT 2009, 9 th June , Venice 7

ISOCHRONIZATION LEVEL UNTIL THE PHASE VARIES WITHIN 20 DEG, THE MAGNETIC FIELD HAS TO

ISOCHRONIZATION LEVEL UNTIL THE PHASE VARIES WITHIN 20 DEG, THE MAGNETIC FIELD HAS TO MATCH THE ISOCHRONOUS ONE WITH A PRECISION OF ± 5 GAUSS (|ΔB/B|<10 -4) HIAT 2009, 9 th June , Venice 8

RF CAVITY DESIGN Emax= 15 MV/m f. RF = 98 MHz, 4 th harmonic

RF CAVITY DESIGN Emax= 15 MV/m f. RF = 98 MHz, 4 th harmonic 50 k. W power losses estimated HIAT 2009, 9 th June , Venice 9

BEAM DYNAMIC STUDY structural resonance coupling resonance HIAT 2009, 9 th June , Venice

BEAM DYNAMIC STUDY structural resonance coupling resonance HIAT 2009, 9 th June , Venice 10

WHAT APPENDS AT RESONANCE ZONE? Minimal transverse stability plot Solution? Jump these radii… but

WHAT APPENDS AT RESONANCE ZONE? Minimal transverse stability plot Solution? Jump these radii… but energy gain cannot increase too much HIAT 2009, 9 th June , Venice 11

Radial beam envelop in two cases old magnetic design Qr cm cm Qr energy

Radial beam envelop in two cases old magnetic design Qr cm cm Qr energy HIAT 2009, 9 th June , Venice energy 12

AUTOELLIPSE TRANSPORT 950 970 990 930 1000 960 940 PR Ar=0. 2 Ar=0. 1

AUTOELLIPSE TRANSPORT 950 970 990 930 1000 960 940 PR Ar=0. 2 Ar=0. 1 980 920 1010 910 1020 900 1030 Number of turns 1040 R HIAT 2009, 9 th June , Venice 13

VERTICAL BEAM DYNAMIC Vertical beam envelop Axial space phase HIAT 2009, 9 th June

VERTICAL BEAM DYNAMIC Vertical beam envelop Axial space phase HIAT 2009, 9 th June , Venice 14

Trimming C 12 to H 2+: RF and MF change Bo=cost. RF Frequency scales

Trimming C 12 to H 2+: RF and MF change Bo=cost. RF Frequency scales 0, 7 % Two beams mean two different operating RF frequencies small variation of the MF gauss Best solution: coils split into two parts (C 400) HIAT 2009, 9 th June , Venice 15

2 nd way: change only the magnetic field f. RF = cost Magnetic field

2 nd way: change only the magnetic field f. RF = cost Magnetic field difference between C 12 and H 2+ is larger, but RF freq. is kept constant (it needs only the fine tuning) HIAT 2009, 9 th June , Venice gauss 16

Trimming by two correction coils HIAT 2009, 9 th June , Venice 17

Trimming by two correction coils HIAT 2009, 9 th June , Venice 17

GOOD M. FIELD MATCHING MINIMIZING POWER LOSSES CC VALLEY CC 1 Less than 4

GOOD M. FIELD MATCHING MINIMIZING POWER LOSSES CC VALLEY CC 1 Less than 4 KW/COIL MAIN COIL HIAT 2009, 9 th June , Venice 18

MAIN SETTING TO CHANGE BEAM PHASE SLIP CALCULATED BY EO MAGNETIC FIELD MATCHING 12

MAIN SETTING TO CHANGE BEAM PHASE SLIP CALCULATED BY EO MAGNETIC FIELD MATCHING 12 C 6+ H 2+ extraction MAIN COIL : 4586 A/cm 2 4586+53. 7 A/cm 2 CC 1: 104. 47 A/cm 2 8 X 8 cm 2 , Rint=171 cm, Hmin=81 cm >> 1. 32 k. W/coil CC VAL: 395. 1 A/cm 2 5 X 4 cm 2 , Rint=106 cm, Hmin=69 cm >> 3. 24 KW/coil RF SETTING: nu 0=24. 18717 MHz 24. 18587 MHz Δf: 1, 3 KHz TRIMMER RANGE TUNING (~ 6 KHz) HIAT 2009, 9 th June , Venice 19

EXTRACTION LAYOUT VED 1, 2 = 50 k. V Emax = 120 k. V/cm

EXTRACTION LAYOUT VED 1, 2 = 50 k. V Emax = 120 k. V/cm 4 PASSIVE MCs protons ε ~ 60 % REXT =122 cm 260 AMe. V 1 single turn Carbon ions 4 PASSIVE MCs ε ~ 100 % HIAT 2009, 9 th June , Venice 20

BEAM DYNAMIC AT EXTRACTION HIAT 2009, 9 th June , Venice 21

BEAM DYNAMIC AT EXTRACTION HIAT 2009, 9 th June , Venice 21

CURRENT BEAM ESTIMATION Carbon ions by EDs Protons by stripper Transmission efficiency HIAT 2009,

CURRENT BEAM ESTIMATION Carbon ions by EDs Protons by stripper Transmission efficiency HIAT 2009, 9 th June , Venice Ion source 2 m. A Injection line 90 % Central region 5 % (no buncher) acceleration 90% extraction 60% C 100% p P current 80 n. A C current 48 n. A 22

CONCLUSION The final design of SCENT 300 was completed and no other study is

CONCLUSION The final design of SCENT 300 was completed and no other study is expected: the technical drawings of the iron steel are also accomplished out. HIAT 2009, 9 th June , Venice 23

GRAZIE ! HIAT 2009, 9 th June , Venice 24

GRAZIE ! HIAT 2009, 9 th June , Venice 24

Coils parameters Coil Parameters Size 150 x 210 mm 2 Current density 46. 5

Coils parameters Coil Parameters Size 150 x 210 mm 2 Current density 46. 5 amp/mm 2 Inner Radius 1420 mm Distance from the M. P. 70 mm Energy Stored Nominal Current (I) 35 MJ 900÷ 1000 amp Total current (NI) 1. 48 Mamp Max Magnetic field 4. 4 tesla Axial Force -9. 09 MN Average Hoop Stress (peak) 100 (110) MPa Conservative Design HIAT 2009, 9 th June , Venice 25

FORCES EVALUATION ON THE COILS (J X B) Vertical force (N) TOT=-891 tons/coil 1

FORCES EVALUATION ON THE COILS (J X B) Vertical force (N) TOT=-891 tons/coil 1 2 3 4 5 6 12 7 11 10 9 8 Radial force (N) Average=166 tons/coil HIAT 2009, 9 th June , Venice 26

STRESS DISTRIBUTION IN THE COILS HOOP STRESS TENSILE STRESS RADIAL STRESS HIAT 2009, 9

STRESS DISTRIBUTION IN THE COILS HOOP STRESS TENSILE STRESS RADIAL STRESS HIAT 2009, 9 th June , Venice 27

HIAT 2009, 9 th June , Venice 28

HIAT 2009, 9 th June , Venice 28

Summary HIAT 2009, 9 th June , Venice 29

Summary HIAT 2009, 9 th June , Venice 29